Force is in a way defined by stating that it is equal to mass times acceleration. The usefulness of the definition (F=ma) comes from the fact that it is also defined in other terms, like how a mass exerts a force on another mass (F=G*m1*m2/distance_between_m1_and_m2^2) or how the force depends on the electrical charges of particles. Because of that one can calculated how masses move or how charged particles move.
In Integral's proposal you see how the force that a spring exerts depends on how far it is stretched (F=-k*Stretch_length), that can be used to calculate how it makes some mass that is attached to it move. But note that the force changes when the mass moves because the movement changes the stretch length, so you will need calculus to calculate how the mass will move.
To show that F=ma you will first have to define what you mean with a force and than show that that when you increase the force that than the acceleration increases with the same factor if you do not change the mass. You can also show that when you double the mass de acceleration halves.
You can use a spring, but as Integral said it is no so easy to have it exert a constant force, if you drag an object attached to a spring along and make sure the spring does not stretch more and also does not stretch less the force on the object will be constant and it will accelerate (so you will have to walk faster and faster to keep the stretch length constant), you will then have to find a method to measure the acceleration. After you have done this you repeat it while you try to hold the spring’s stretch length at a different length (the length ratio is equal to the ratio between the forces, as you can deduce from F=-k*Stretch_length).